Talks given (this list was exhaustive until around 2011, and since then is a representative selection of topics)
Uniqueness of equilibrium states for geodesic flows in manifolds of nonpositive curvature
Geometry seminar, Yale, March 2016
Dynamics seminar, Michigan, February 2016
We establish results on uniqueness of equilibrium states for geodesic flows on rank one manifolds. This is an application of machinery developed by Vaughn Climenhaga and myself, which applies when systems satisfy suitably weakened versions of expansivity and the specification property. The geodesic flow on a rank one manifold is a canonical example of a non-uniformly hyperbolic flow and I'll explain why it satisfies our hypotheses. Our methods are completely different from those used by Knieper in his seminal proof that there is a unique measure of maximal entropy in this setting. This is joint work with Keith Burns (Northwestern), Vaughn Climenhaga (Houston) and Todd Fisher (Brigham Young).
Entropy for generalised beta-transformations
British Mathematics Colloquium, Queen Marys (London), April 2014
Pure Mathematics Colloquium, St. Andrews, April 2014
Generalised beta-transformations are the class of piecewise continuous
interval maps given by taking the beta-transformation x↦βx (mod1),
where β > 1, and replacing some of the branches with branches of
constant negative slope. We would like to describe the set of beta for
which these maps can admit a Markov partition. We know that beta (which
is the exponential of the entropy of the map) must be an algebraic
number. Our main result is that the Galois conjugates of such beta have
modulus less than 2, and the modulus is bounded away from 2 apart from
the exceptional case of conjugates lying on the real line. This
extends an analysis of Solomyak for the case of beta-transformations,
who obtained a sharp bound of the golden mean in that setting.
I will also describe a connection with some of the results of Thurston's fascinating final paper, where the Galois conjugates of entropies of post-critically finite unimodal maps are shown to describe an intriguing fractal set. These numbers are included in the setting that we analyze.
Equilibrum states for certain robustly transitive diffeomorphisms
Ergodic theory and dynamical systems seminar, University of Warwick, April 2014
We establish results on uniqueness of equilibrium states for the
well-known Mane examples of robustly transitive diffeomorphisms. This
is an application of machinery developed by Vaughn Climenhaga and
myself, which applies when systems satisfy suitably weakened versions
of expansivity and the specification property. The Mane examples
are partially hyperbolic maps of the 3-torus, and I'll explain why
these maps satisfy our hypotheses. This is joint work with Vaughn
Climenhaga (Houston) and Todd Fisher (Brigham Young).
Coding Sequence Density Estimation via Topological Pressure
ICIAM conference, Ohio State MBI, May 2014
I will describe an approach to coding sequence (CDS) density estimation
in genomic analysis introduced recently by myself and David Koslicki.
Our approach is based on the topological pressure, which is a measure
of ‘weighted information content’ adapted from ergodic theory. We use
the topological pressure (with suitable training data) to give ab
initio predictions of CDS density on the genomes of Mus Musculus,
Rhesus Macaque and Drosophila Melanogaster. While our method is not
sufficiently precise to predict, for example, the exact locations of
genes, we demonstrate that our method gives reasonable estimates for
the ‘coarse scale’ problem of predicting CDS density. This is joint
work with David Koslicki (Oregon State).
Large deviations and horseshoes for S-gap shifts.
IUPUI, October 2013
This is joint work with Vaughn Climenhaga and Kenichiro Yamamoto. I
will explain how we establish the large deviations principle for the
family of S-gap shifts. Key to our approach is a 'horseshoe theorem'
which allows us to approximate invariant measures by ergodic measures
supported on sofic subshifts of the S-gap shift. Although I will focus
on the concrete example of S-gap shifts for ease of exposition, our
large deviations result actually applies much more generally, and is
based on machinery developed by Climenhaga and myself to prove
uniqueness of equilibrium states in various different 'non-uniform'
Intrinsic ergodicity, orbit gluing and S-gap shifts
Midwest Dynamics Conference, October 2013
This talk is based on a series of papers by Vaughn Climenhaga
(Houston) and myself where we develop a new approach to prove
uniqueness of equilibrium measures for dynamical systems with
various non-uniform structures.
One class of model examples that motivated our results is the
family of S-gap shifts. The S-gap shifts are a natural family of
symbolic spaces which are easy to define but can be challenging to
study! For a fixed subset S of the natural numbers, the
corresponding S-gap shift is the collection of binary sequences
which satisfy the condition that the length of every run of
consecutive 0's is a member of S. Examples are the even shift (we
let S be the even numbers) and the prime gap shift (we let S be
the prime numbers).
The key difficulty in the study of S-gap shifts is a spectacular
failure of the Markov property, and we develop techniques to deal
with this. These techniques can be adapted to apply to many other
interesting dynamical systems beyond the well understood uniformly
hyperbolic case (e.g. beta-shifts, interval maps with parabolic
fixed points, non-uniformly expanding maps in higher dimensions,
some partially hyperbolic examples).
I will explain our approach and motivations focusing on the example of
S-gap shifts, building up to our result that 'Every subshift factor of
an S-gap shift (or a beta-shift) is intrinsically ergodic'. If time
permits, I will also describe a brand new result by Climenhaga,
myself and Kenichiro Yamamoto (Tokyo Denki University) which
establishes a large deviations principle for S-gap shifts.
A 'horseshoe' theorem in symbolic dynamics via single sequence techniques.
Mathematical Congress of the Americas, August 2013
For a broad class of symbolic dynamical systems without the Markov
property, including the coding spaces of many piecewise continuous
interval maps, we show how to approximate an arbitrary ergodic measure
with a measure of almost the same entropy supported on a sofic
subshift. This is interpreted as a symbolic analogue of a `hyperbolic
horseshoe' theorem. In addition to the intrinsic interest of this
result as a structure theorem, it can be a useful tool in large
deviations theory and multifractal analysis. I will discuss two ways to
establish this result, both based on surgery on a single generic orbit.
One proof is based on Ornstein's d bar metric, and the other is based
on the theory of Kolmogorov complexity. Both techniques can be
explained in a simple and intuitive way.
Equilibrium states and large deviations principles for beta-shifts, S-gap shifts, and beyond.
Conference on Thermodynamic Formalism, PUC (Chile), July 2013
I will give an overview, and report on recent progress, for a long-term
project joint with Vaughn Climenhaga concerning measures of maximal
entropy and equilibrium states for a large class of dynamical systems
with a 'non-uniform orbit structure', including piecewise continuous
and parabolic interval maps, and some higher dimensional partially
I will explain our approach and motivations focusing on the
illustrative example of S-gap shifts, building up to our result that
'the level 2 large deviations principle holds for every S-gap shift',
which was recently obtained by Climenhaga, myself and Kenichiro
Yamamoto. If time permits, I will also describe our application to
partially hyperbolic examples which is joint work with Todd Fisher.
Uniqueness of equilibrium states: Beta-shifts, the Bowen property and Beyond
Maryland-Penn State Workshop on Dynamical Systems, Maryland, April 2011
Dynamics seminar, CUNY, May 2011
This joint work with Vaughn Climenhaga (Maryland) establishes uniqueness of equilibrium states for
1) a large class of shift spaces which includes every beta-shift;
2) a large class of potential functions which strictly includes those with the Bowen property.
As an application, our method yields new results in the theory of
thermodynamic formalism for piecewise monotonic interval maps. Our
method allows us to handle a variety of systems without a Markov
structure, and it covers a class of potentials that are well behaved
away from a 'small' set; for example, an indifferent fixed point or a
point of discontinuity. This work extends the techniques which we
developed in a recent preprint, available at http://arxiv.org/abs/1011.2780,
which gave a positive answer to the question 'Is every subshift factor
of a beta-shift intrinsically ergodic?'. This question was included in
Mike Boyle's article 'Open problems in symbolic dynamics', and was the
original motivation for the development of these techniques.
Distinguished invariant measures for Beta-shifts and their factors.
University of Washington, Seattle, April 2011
This talk is based on joint work with Vaughn Climenhaga
(Maryland), in which we show that every shift space which is a factor
of a beta-shift has a unique measure of maximal entropy. This provides
an affirmative answer to Problem 28.2 of Mike Boyle's article 'Open
problems in symbolic dynamics'.
A measure of maximal entropy is a measure which witnesses the greatest
possible complexity in the orbit structure of a topological dynamical
system. Establishing when a system has a unique measure of maximal
entropy is a fundamental topic in ergodic theory and has been studied
extensively since the 1960's. The beta-shifts are a class of symbolic
spaces with an extremely rich structure and a profound connection to
Our method actually applies to a rather large general class of shift
spaces, and can also be applied to non-symbolic systems. We have
recently extended our results to establish uniqueness of equilibrium
measures for a large class of potential functions. We obtain new
results in the setting described above, and even in the case of the
full shift. I will give a detailed explanation of the problems
described above and their motivation. I will also describe, via a
detailed description of the beta-shift, the key ideas behind our method.
'Subshift factors of the beta-shift
are intrinsically ergodic'
University of Richmond (2010 AMS Fall Southeastern
meeting), November 2010
Penn State Workshop in Dynamical Systems and Related
Topics, October 2010
This talk is based on joint work with Vaughn Climenhaga (Maryland), in
which we show that every subshift factor of a beta-shift has a unique
measure of maximal entropy. This provides an affirmative answer to
Problem 28.2 of Mike Boyle's article 'Open problems in symbolic
dynamics'. I'll explain the problem and its relation to existing
results and give an idea of how our approach works. Our techniques are
essentially new, and allow us to deal with dynamical systems which are
a long way from being Markov. I will describe a broad and natural class
of shift spaces to which our results apply.
'Topological pressure for non-compact sets, Kamae entropy and Kolmogorov complexity'
Logic Seminar, Pennsylvania State University, November 2010
For compact spaces, the theory of topological pressure and equilibrium
states is a cornerstone of modern ergodic theory. It has long been
thought desirable to generalize this theory to non-compact spaces. I
will give a brief over-view of the various approaches to this problem
in the literature and give an elementary alternative definition of
topological pressure in the non-compact setting. It turns out that this
definition is a generalization of the Kamae entropy. The definition
assigns a non-negative number to each point in the space and can be
interpreted as a sort of complexity. In Cantor space, this quantity is
related to the Kolmogorov complexity. I will attempt to give an
accessible explanation of the dynamical systems context of this theory.
I will then describe some results by Brudno, Kamae, Van Lambalgen and
White to illustrate the connection with Kolmogorov complexity and to
demonstrate why this may be of interest to Logicians.
'Subshift factors of the beta-shift
are intrinsically ergodic'
Penn State Dynamics conference October 2010, South-Eastern AMS meeting November 2010
This talk is based on joint work with Vaughn Climenhaga,
in which we show that every subshift factor of a $\beta$-shift has a
unique measure of maximal entropy. This provides an affirmative answer
to Problem 28.2 of Mike Boyle's article `Open problems in symbolic
dynamics'. I'll explain the problem and its relation to existing
results and give some idea of how our approach works. I'll also discuss
some other examples of symbolic spaces where our technique can be
'A criterion for topological entropy to decrease under normalised Ricci flow'
Versions of this talk were given at Penn
State, Yale, Northwestern, Maryland and Rice
In 2004, Manning showed that the topological entropy of the geodesic
ﬂow for a surface of negative curvature decreases as the metric evolves
under the normalised Ricci ﬂow. It is an interesting open problem,also
due to Manning, to determine to what extent such behaviour persists for
dimensional manifolds. I will describe a curvature condition on the
metric under which monotonicity of the topological entropy can be
established for a short time. In particular, this criterion applies to
metrics of negative sectional curvature which are in the same
conformal class as a metric of constant negative sectional curvature.
'Interpretation and applications of topological entropy in geometry'
Penn State, Working Geometry seminar, February 2010
Interpretation: The topological entropy is one of the key invariants in
the theory of dynamical systems. When the dynamical system is a
geodesic flow on a negatively curved manifold, it is good to know that
the topological entropy has a very natural formulation as a geometric
quantity. It is the exponential growth rate of volume in the universal
cover. I'll sketch the classic proof of this fact which is due to
Manning. Application: I'll sketch A. Katok's classic proof of his
fascinating result which tells us that the topological entropy can be
used to characterize which metrics on a surface are hyperbolic. More
precisely, the topological entropy of the geodesic flow is minimised at
the constant curvature metrics.
set for the beta transformation carries full topological entropy (= log
beta) and full Hausdorff dimension (=1)'
Penn State, Dynamical Systems seminar, October 2009, Boston University, Dynamical Systems seminar, October
The beta-transformation f(x) = beta x (mod 1) has been widely studied
since its introduction by Renyi in 1957. The sustained interest in the
study of the beta-transformation arises from its connection with number
theory and its special role as a model example of a one-dimensional
expanding dynamical system which admits discontinuities.
We show that for the beta transformation, the set of points for which
the Birkhoff average of a continuous function does not exist (which we
call the irregular set) is either empty or has full topological entropy
and Hausdorff dimension.
This result follows from a corresponding result about dynamical systems
which satisfy a topological dynamical property which we call almost
specification. It turns out that every beta-shift satisfies almost
specification, and we will explain how this works.
'Another look at topological pressure for non-compact sets'
Seminar (part of themed semester in ergodic theory), University of Surrey, March 2009
It has long been thought desirable to generalise the standard theory of
topological pressure and equilibrium states to non-compact spaces.
Notably, Sarig developed the theory of Gurevic pressure for countable
state shifts. This theory has many applications, particularly in the
study of non-uniformly hyperbolic systems, where inducing schemes lead
naturally to the study of countable state shifts.
In another direction, Bowen defined topological entropy for non-compact
sets as a characteristic of dimension type. The study of topological
entropy for the multifractal decomposition of Birkhoff averages (for
example) is a well accepted goal in its own right. Pesin and Pitskel
contributed a definition of topological pressure for non-compact sets
which generalises the Bowen definition.
We give an elementary alternative definition of topological pressure in
the non-compact setting. The definition is made via a suitable
variational principle leading to an alternative definition of
equilibrium state. We derive some properties of the new topological
pressure and compare it with the other definitions. We give a simple
example which illustrates the difference in the thermodynamic
properties of the new pressure and the Pesin and Pitskel pressure. We
describe an example taken from the multifractal analysis of the
Lyapunov exponent for the Manneville-Pomeau family of maps, which seems
particularly well adapted to our new framework. We hope that the new
theory will have useful applications and we mention some aspirations in
'The irregular set for the beta transformation carries full topological entropy (= log beta)'
London Mathematical Society one day ergodic theory meeting, University of Warwick, January 2009;
Dynamical Systems Seminar, Northwestern University, October 2008
A recent weakening of the specification property provides new tools to
study interesting systems beyond the scope of uniformly hyperbolic
dynamics such as the beta-transformation. This property was introduced
by Pfister and Sullivan as the g-almost product property. The version
we study is a priori slightly weaker and we rename it the almost
specification property. We show that for dynamical systems with almost
specification, the set of points for which the Birkhoff average of a
continuous function does not exist (which we call the irregular set) is
either empty or has full topological entropy.
Every beta-shift satisfies almost specification and we show that the
irregular set for any beta-shift or beta-transformation is either empty
or has full topological entropy and Hausdorff dimension.
The talk is in three parts. Firstly, we give some history on results
about the topological entropy and Hausdorff dimension of the irregular
set. Secondly, we discuss our abstract results and try to give some
intuition as to why they are true. Thirdly, we discuss in detail the
application to the beta-transformation. In particular, we give some
intuition on the almost specification property and show why it is
satisfied by the beta-transformation.
'The Liouville entropy of a 3-manifold is not monotonic along the Ricci flow'
Maryland-Penn State Workshop on Dynamical Systems, Penn State, October 2008
In 2004, Manning used an important formula of Katok, Knieper and Weiss
to prove that as the metric on a negatively curved surface evolves
under the (normalised) Ricci flow, the topological entropy of the
geodesic flow decreases. In contrast, we observe that an example
of Flaminio can be used to show that the Liouville entropy can either
increase or decrease along a Ricci flow in a neighbourhood of a
particular 3-manifold of constant negative curvature. We will introduce
this topic, explain our observation, and recall some of the interesting
and challenging open questions in this area.
'The Irregular Set for Maps with the Specification Property Carries Full Topological Pressure'
Maryland-Penn State Workshop on Dynamical Systems, University of Maryland, March 2008
We describe a result that applies to any dynamical system (X, T) with
the specification property. Systems satisfying specification include
any continuous map which is a factor of a topologically mixing shift of
finite type and any topologically mixing continuous interval map.
We show that, for a generic function f on X, the irregular set of f
(the set of points for which the Birkhoff average of f does not exist)
carries full topological pressure (in the sense of Pesin and Pitskel).
Topological pressure is interpreted as a ‘weighted’ dynamical size, so
the result says that the irregular set is as ‘large’ as it can be in an
appropriate topological sense. This result may be surprising given that
the irregular set has zero measure with respect to any invariant
measure. In the case of topological entropy, this phenomenon was
first noticed for Bernoulli shifts by Pesin and Pitskel and generalised
to a variety of uniformly hyperbolic systems by Barreira and Schmeling.
As an application, we show that the irregular set for a suspension flow
over a continuous map with specification carries full topological
entropy, generalising a result of Barreira and Saussol.
'A Thermodynamic Definition of Topological Pressure for Non-Compact Sets'
Dynamics Seminar, Warwick Mathematics Institute, January 2008; Dynamics Seminar, Manchester University, November 2007
In the 80's, Pesin and Pitskel defined topological pressure for
non-compact sets as a characteristic of dimension type, generalising a
definition of topological entropy introduced by Bowen. We give an
alternative definition of topological pressure in the non-compact
setting via a suitable variational principle. We derive some properties
of the new topological pressure and compare them with the properties of
the Pesin and Pitskel pressure. We describe a simple example which
illustrates the difference in the thermodynamic properties of the two
quantities. We conclude with an example taken from the multifractal
analysis of the Lyapunov exponent for the Manneville-Pomeau family of
maps, which seems particularly well adapted to our new framework.
'The Irregular Set for Maps with the Specification Property carries Full Entropy'
Conference ‘Chaotic Properties of Dynamical Systems’, Warwick Mathematics Institute, August 2007
The content was similar to 'The Irregular Set for Maps with the
Specification Property Carries Full Topological Pressure' (but less
'The Multifractal Miracle: Multifractal Analysis in Symbolic Dynamics'
Postgraduate Seminar, Warwick Mathematics Institute, November 2006
This was a talk for a general postgraduate audience.
I offer two abstracts for the talk, the second being of a more technical and precise nature:
Abstract Version 1: We are interested in the average value of a
function along the orbit (under a continuous transformation) of a
point. This quantity is known as the Birkhoff (or ergodic) average.
Does this average exist? What values does it take? It has been known
since the 1930's that from the point of view of measure theory the
Birkhoff average is very well behaved. However, from the topological
viewpoint, a priori, this average behaves rather badly. However,
by the so called 'multifractal miracle', one can say a surprising
amount about the destination of the Birkhoff sum. In the context of
symbolic dynamics, I will describe the 'multifractal miracle' in a way
accessible to a general postgraduate audience.
Abstract Version 2: Birkhoff's ergodic theorem tells us that for an
integrable function f on a dynamical system, the Birkhoff sum converges
to $\int f d m$ almost everywhere with respect to an ergodic measure
$m$. However, there are simple examples of systems such as the
Bernoulli shift which admit uncountably many distinct ergodic measures.
Thus, for a given point, there may be uncountably many possibilities
for its ergodic average. Indeed, its ergodic average may not exist at
all. What can be said about where the Birkhoff sum 'goes'? How `large'
is the set of points whose ergodic average takes a given value? I will
explain some results in this direction in the case of symbolic dynamics
and a variety of systems that admit codings. The results will require
an explanation of the theory of equilibrium/ Gibbs measures in symbolic
dynamics and a discussion of characteristics of 'dimension type'. I aim
to make the talk accessible to as wide an audience as possible, so I
will define precisely any technical terms that I use, including
ergodicity, Birkhoff sum and the Bernoulli shift.